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The canonical crystal is a highest weight crystal of highest weight
Statement
Let and let be the crystal of from The Kashiwara lattices and and their generating sets, which is a crystal basis by The grand loop: existence of the highest weight crystal bases. Then is a highest weight crystal of highest weight in the sense of Highest weight elements, lowering-generated sets and highest weight crystals:
(i) is a highest weight element of weight : and for every ;
(ii) : every is an iterated lowering image ;
(iii) is the only highest weight element of : , and for every and every nonzero homogeneous there is with .
No choice principle is used.
Facts & Assumptions
Given: A dominant integral label (Kac moody integral and dominant integral weights), the simple integrable highest weight module with highest vector (The integrable quantum highest weight module exists and is unique), its lattice and basis (The Kashiwara lattices and and their generating sets), and the residue .
Crystal basis of (The grand loop: existence of the highest weight crystal bases, The Kashiwara lattices and and their generating sets): is a crystal basis of ; is a free -module for every , and since is generated over by the lowering words applied to and no nonempty word has weight , is free of rank generated by ; .
The lattice and basis of highest weight (The Kashiwara lattices and and their generating sets): is generated over by the lowering words and ; moreover for one has and .
Crystal-lattice axioms (Crystal lattices, crystal bases and their crystals): is a -basis of with , the operators satisfy on existing edges and , in the form .
Crystal graph conventions (The crystal graph, , and the weight function): maps a vertex of weight with to a vertex of weight ; is finite, and exactly for .
Structure of (The integrable quantum highest weight module exists and is unique, Quantum Verma modules , highest weight vectors, and the simple highest weight quotient ): has label-weight support contained in and finite-dimensional label-weight spaces; it is generated by under , and its weight space is one-dimensional, spanned by the image of , because is the simple graded quotient of the Verma module whose highest line maps onto it.
Weight modules and integrability (Quantum weight modules, weights in , and integrability) and the Kashiwara operators (The Kashiwara operators and of an integrable module) supply the weight grading and the string structure on which [F2]-[F4] operate.
The definition of a highest weight element and of (Highest weight elements, lowering-generated sets and highest weight crystals).
Proof
The top residue. By [F1], is free of rank one with generator , so its residue space is one dimensional and by [F3]; in particular . If for some , then by [F4] it is an element of and is the residue of a nonzero homogeneous vector of of weight ; but by [F5], a contradiction since . Hence for all , and is a highest weight element of weight , proving (i).
Lowering-word generation. Clause (c) of [F2] states for . Induction on the height proves that every is an iterated lowering image of : for this is step 1.1, and for the formula exhibits with of strictly smaller height, to which the induction hypothesis applies. Hence , proving (ii).
Killing by all . Let and let be nonzero with for every . Since is a -basis of this space by [F3] and [F1] shows it is finite (it has elements), is a finite sum with coefficients . Fix : the nonzero elements among , , lie in and are pairwise distinct by the partial-inverse axiom [F3], hence linearly independent in the -vector space ; the relation therefore forces for every with . This holds for every . Now let ; by step 2.1 is a lowering word of positive length from (since ), so for the last letter , and then by [F3]; hence every occurs among the terms with for some , so all and , a contradiction. This proves (iii).
Conclusion. Steps 1.1, 2.1 and 3.1 establish (i), (ii) and (iii), so has a highest weight element of weight and : it is a highest weight crystal of highest weight in the sense of [F7]. All arguments used finite sums and the fixed basis ; no choice principle was used.
Depends on
- Highest weight elements, lowering-generated sets and highest weight crystals
- The Kashiwara lattices $\mathcal L(\lambda)$ and $\mathcal L(\infty)$ and their generating sets
- The grand loop: existence of the highest weight crystal bases
- Crystal lattices, crystal bases and their crystals
- The crystal graph, $\varepsilon_i$, $\varphi_i$ and the weight function
- The Kashiwara operators $\tilde e_i$ and $\tilde f_i$ of an integrable module
- Kac moody integral and dominant integral weights
- The integrable quantum highest weight module exists and is unique
- Quantum Verma modules $M(\lambda)$, highest weight vectors, and the simple highest weight quotient $L(\lambda)$
- Quantum weight modules, weights in $P$, and integrability
Used by
- The regular-partition label convention and the Mullineux crystal involution Definition
- The empty partition generates an integrable highest weight submodule of highest weight Λ₀ Proposition
- Highest weight components in a tensor product crystal Theorem
- Simple and indecomposable-projective crystals agree with B(Λ) Theorem
- The empty component is the highest weight crystal B(Λ₀) Theorem
- Uniqueness: crystal bases of integrable modules decompose into highest weight crystals Theorem
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Sources
- Masaki Kashiwara, On crystal bases of the q-analogue of universal enveloping algebras, Duke Math. J. 63 (1991), no. 2, 465-516 (standard reference, not scraped)
- Richard Borcherds, Mark Haiman, Theo Johnson-Freyd, Nicolai Reshetikhin and Vera Serganova, Berkeley Lectures on Lie Groups and Quantum Groups (book-length lecture notes, last updated 18 January 2024) (standard reference, not scraped)
- Kyeonghoon Jeong, Seok-Jin Kang and Masaki Kashiwara, Crystal Bases for Quantum Generalized Kac-Moody Algebras, arXiv:math/0305390 (standard reference, not scraped)